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Hooke’s Law for a Wire. A wire of lengthl0and cross-sectional areasupports a hanging weight W.

  1. Show that if the wire obeys Eq. (11.7), it behaves like a spring of force constantAYl0, where Yis Young’s modulus for the wire material.
  2. What would the force constant be for alength of 16-gauge (diameter = 1.291 mm) copper wire? See Table 11.1.
  3. What wouldhave to be to stretch the wire in part (b) by 1.25 mm?

Short Answer

Expert verified
  1. It is proved thatk=YAl0
  2. The force constant is1.92×105Nm.
  3. Weight is2.4×102N .

Step by step solution

01

Use of equation 11.10

Consider the formulas:

Y=Tensile stressTensile strain=F⊥/AΔI/I0=F⊥ΔVI0A

Here,F⊥is force perpendicular to cross section,∆l is elongation,l0 Original length and A is cross sectional area of object.
02

Identification of given data

Length of wire is l0

Cross sectional area of object is A

Weight of object is W

03

Prove that AYI0

(a)

Here we have to prove:k=YAI0

Our goal is to expressF⊥∆lbecause that is the force constant which we can see in formula (11.7)

Now, by formula (11.7) which is given by,

Hooke'slaw=StressStrain

Here, stress is measure of forces applied to body. Strain is measure of how much deformation results from stress.

Now, from equation (1), we have,

Y=F⊥AI0ΔIYAI0=F⊥ΔINow,weknowthatF⊥∆l=kSo,aboveequationbecomesk=YAI0

Hence proved.

04

Find the force constant be for a 75.0 cm  length of 16-gauge (diameter = 1.291mm ) copper wire

(b)

From part (a) we have,

k=YAI0

Now, for copper wire above equation becomes

k=YCuAI0 (2)

Now, YCu=11×1010

Determine the area:

A=πr2=π1.29×10−32=1.31×10−6m2

Now, by substituting all the numerical values in equation (2).

k=11×10101.31×10−6m20.75m=1.92×105Nm

Hence, the force constant is1.92×105Nm.

05

Find  to stretch the wire in part (b) by

(c)

To find the weight W for given∆lis given by,

k=W∆lW=kΔlW=1.92×105N/m⋅1.25×10−3mW=2.4×102

Hence, Weight is2.4×102N .

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